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CN1087504C - High frequency static induction transistor having high output - Google Patents

High frequency static induction transistor having high output Download PDF

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Publication number
CN1087504C
CN1087504C CN96110070A CN96110070A CN1087504C CN 1087504 C CN1087504 C CN 1087504C CN 96110070 A CN96110070 A CN 96110070A CN 96110070 A CN96110070 A CN 96110070A CN 1087504 C CN1087504 C CN 1087504C
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region
gate
regions
guard ring
source
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CN1144402A (en
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西泽润一
本谷薰
伊藤彰
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Digital multi Limited by Share Ltd
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Zaidan Hojin Handotai Kenkyu Shinkokai
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/01Manufacture or treatment
    • H10D30/012Manufacture or treatment of static induction transistors [SIT], e.g. permeable base transistors [PBT]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/202FETs having static field-induced regions, e.g. static-induction transistors [SIT] or permeable base transistors [PBT]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/102Constructional design considerations for preventing surface leakage or controlling electric field concentration
    • H10D62/103Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices
    • H10D62/105Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices by having particular doping profiles, shapes or arrangements of PN junctions; by having supplementary regions, e.g. junction termination extension [JTE] 
    • H10D62/106Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices by having particular doping profiles, shapes or arrangements of PN junctions; by having supplementary regions, e.g. junction termination extension [JTE]  having supplementary regions doped oppositely to or in rectifying contact with regions of the semiconductor bodies, e.g. guard rings with PN or Schottky junctions
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/20Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/23Electrodes carrying the current to be rectified, amplified, oscillated or switched, e.g. sources, drains, anodes or cathodes
    • H10D64/251Source or drain electrodes for field-effect devices
    • H10D64/252Source or drain electrodes for field-effect devices for vertical or pseudo-vertical devices
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/20Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/27Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
    • H10D64/311Gate electrodes for field-effect devices
    • H10D64/411Gate electrodes for field-effect devices for FETs

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Abstract

一种击穿电压高的凹型静态晶体管,包括:设置在n+型漏区的n型沟道区,在沟道槽中的P+型伸长栅区,在沟道区形成的和栅区平行的n+型伸长区,其中每一个设置在栅区之间,在沟道区中的围绕栅区的P+型保护环区。伸长栅区在两边与保护环区耦连,最外部的伸长栅区在纵向与保护环区分别耦连,以增加器件的击穿电压。栅和源接触点仅在保护环区彼此相对设置,以减少栅漏区之间和栅源区之间的寄生电容。

Figure 96110070

A concave static transistor with high breakdown voltage, comprising: an n-type channel region arranged in an n + -type drain region, a p + -type elongated gate region in the channel groove, and a gate region formed in the channel region Parallel n + -type elongated regions, each of which is disposed between the gate regions, and a p + -type guard ring region surrounding the gate regions in the channel region. The elongated gate region is coupled with the guard ring region on both sides, and the outermost elongated gate region is respectively coupled with the guard ring region in the longitudinal direction, so as to increase the breakdown voltage of the device. The gate and source contacts are arranged opposite to each other only in the guard ring region to reduce the parasitic capacitance between the gate-drain region and between the gate-source region.

Figure 96110070

Description

高输出功率的高频静态感应晶体管High Frequency Static Sense Transistor for High Output Power

本发明涉及静态感应晶体管(SIT),特别涉及高输出功率的高频凹栅型或侧栅型静态感应晶体管。The invention relates to a static induction transistor (SIT), in particular to a high-frequency concave-gate or side-gate static induction transistor with high output power.

参看图20叙述现有技术的SIT。图20(A)表示表面栅型SIT,它包括,作为漏区的n+衬底101,设置在衬底101上面作为沟道区的外延层102,在n型外延层102表面上形成的n+源区103和p+栅区104。按照这种表面栅结构,通过减少栅电阻以便改善高频特性。已提供在大约1GHz工作的表面栅型SIT。由于设置扩散深度为2-3μm或更深的P+栅区104,则当n型外延层102的厚度是20μm时,可能获得200-300V的击穿电压,同样,当n型外延层102的厚度是6μm时,可以获得600V的击穿电压。Referring to Fig. 20, the prior art SIT will be described. Fig. 20 (A) shows surface gate type SIT, and it comprises, as drain region n + substrate 101, is arranged on the substrate 101 top as the epitaxial layer 102 of channel region, on the surface of n type epitaxial layer 102 forms n + source region 103 and p + gate region 104. According to this surface gate structure, the high frequency characteristics are improved by reducing the gate resistance. Surface-gate SITs operating at about 1 GHz have been provided. Since the P + gate region 104 with a diffusion depth of 2-3 μm or deeper is set, when the thickness of the n-type epitaxial layer 102 is 20 μm, a breakdown voltage of 200-300V may be obtained. Similarly, when the thickness of the n-type epitaxial layer 102 When it is 6μm, a breakdown voltage of 600V can be obtained.

已经提出如图20(B)和图20(C)所示的凹栅型和侧栅型SIT作为进一步改善高频特性的结构。在凹栅型SIT中,在n型外延层102中形成槽105。在槽105的底上形成P+栅区106。在侧栅型SIT中在槽107的两个拐角形成P+栅区108,槽107是在n外延层102中形成的。因为这两种SIT和表面栅型SIT相比,减少了栅-源间的电容量Cgs和栅-漏间的电容量Cgd,所以功率增益几乎上升到UHF频段的上限。在凹栅型SIT的情况,外延层102的厚度是大约6-10μm,在1-3GHz的功率增益是7-10db,并且器件可能在几GHZ的最大振荡频率fmax下工作,增益变成1(0 dB)。A recess gate type and a side gate type SIT as shown in FIG. 20(B) and FIG. 20(C) have been proposed as structures for further improving high-frequency characteristics. In the recessed gate type SIT, grooves 105 are formed in n-type epitaxial layer 102 . A P + gate region 106 is formed on the bottom of the trench 105 . In the side gate type SIT, P + gate regions 108 are formed at both corners of the trench 107 formed in the n epitaxial layer 102 . Because the two SITs reduce the gate-source capacitance C gs and the gate-drain capacitance C gd compared with the surface gate SIT, the power gain almost rises to the upper limit of the UHF frequency band. In the case of a concave gate type SIT, the thickness of the epitaxial layer 102 is about 6-10 μm, the power gain at 1-3 GHz is 7-10 db, and the device may work at the maximum oscillation frequency f max of several GHZ, the gain becomes 1 (0dB).

为提高高频特性,要减少栅-源电容Cgs和栅-漏电容Cgd。为减少Cgd,可以把P+栅区106的扩散深度Xj作浅。由于Cgd随栅区和漏区之间的距离增大而相反地增加,可把n外延层102作厚,以便减少Cgd。但是,如果把n外延层102作厚,则由于电子从源区到漏区引的传输时间影响,结果减少增益。因此,Cgd和fmax对n外延层102的厚度有一折衷关系。In order to improve high-frequency characteristics, gate-source capacitance C gs and gate-drain capacitance C gd should be reduced. To reduce C gd , the diffusion depth Xj of the P + gate region 106 can be made shallow. Since C gd increases inversely as the distance between the gate region and the drain region increases, the n epitaxial layer 102 can be made thicker in order to reduce C gd . However, if the n-epitaxial layer 102 is made thick, the gain is reduced as a result due to the influence of the transit time of electrons from the source region to the drain region. Therefore, C gd and f max have a trade-off relationship with the thickness of the n-epitaxial layer 102 .

为了增加栅-漏间的击穿电压BVgd,可以增加Xj。但是,可减少栅区和漏区之间的距离来增加Cgd。也就是说,BVgd和Cgd与P+栅区106扩散厚度Xj有一折衷关系。如上所述,高频特性与击穿电压有很大关系。BVgd是栅漏区之间P-n结的反向击穿电压,由此,确定适于漏区的最大电压(击穿电压)。In order to increase the gate-drain breakdown voltage BV gd , Xj can be increased. However, the distance between the gate and drain regions can be reduced to increase C gd . That is to say, there is a trade-off relationship between BV gd and C gd and the diffusion thickness Xj of the P + gate region 106 . As mentioned above, high frequency characteristics have a great relationship with breakdown voltage. BV gd is the reverse breakdown voltage of the Pn junction between the gate-drain region, thereby determining the maximum voltage (breakdown voltage) suitable for the drain region.

实际的凹栅型SIT的BVgd比由平面结确定的理论击穿电压要低。给栅和漏区之间的P-n结加电压,直到击穿,然后用红外线辐射显微镜观察SIT的表面。发现在P+栅区106的最外缘部分的温度升高因此,在最外面部分产生的球面形或圆柱形的结区的击穿电压降低而不是在栅和漏区之间的平面结区(获得理论击穿电压的部分)击穿电压降低。The BV gd of the actual concave-gate SIT is lower than the theoretical breakdown voltage determined by the planar junction. Apply a voltage to the Pn junction between the gate and drain until it breaks down, and then observe the surface of the SIT with an infrared radiation microscope. It is found that the temperature increases at the outermost portion of the P + gate region 106. Therefore, the breakdown voltage of the spherical or cylindrical junction region created at the outermost portion instead of the planar junction region between the gate and drain regions decreases. (The part where the theoretical breakdown voltage is obtained) The breakdown voltage decreases.

因为SIT的输出功率与漏电压和漏电流成比例的增加,为了实现高频大输出功率的器件,采用由栅漏区之间的厚度确定的理论击穿电压,但不降低高频特性,进行最佳设计。但是,实际的BVgd要低于理论击穿电压,因此,为了提供高频大输出功率的凹栅型SIT,应使BVgd增大到算出的理论击穿电压。对于侧栅型SIT要进行同样的处理。Because the output power of the SIT increases in proportion to the drain voltage and the drain current, in order to realize a device with high frequency and high output power, the theoretical breakdown voltage determined by the thickness between the gate and drain regions is adopted, but the high frequency characteristics are not reduced, and the best design. However, the actual BV gd is lower than the theoretical breakdown voltage. Therefore, in order to provide a concave grid SIT with high frequency and high output power, the BV gd should be increased to the calculated theoretical breakdown voltage. The same process is performed for the side gate type SIT.

其次,参照附图21(A)简略叙述SIT中的栅和源极结构。在用虚线包围区中(元件区120),平行地设置P+栅区和n+源区,栅极108和源极109分别设置在P+栅区和n+源区上。铝(A1)栅接触点110和铝(A1)源接触点111形成在最外面的元件区120上。栅接触点110和每一栅电极108之间的连接区112用右上斜线表示,源接触点111和每一源极109之间的连接部分用左下斜线表示。如图21(B)所示,在外延层102上面形成氧化膜114,在氧化膜114上面设置栅接触点11。同样,虽然没有表示,在氧化膜114上面,也形成源接触点111。上述接触点结构中,在栅和漏区之间的击穿电压虽然决定于每个A1接触点下面氧化层的厚度和质量,但是它是大约200-300V。Next, the gate and source structures in the SIT will be briefly described with reference to FIG. 21(A). In the area surrounded by a dotted line (element area 120), the P + gate area and the n + source area are arranged in parallel, and the gate 108 and the source 109 are respectively arranged on the P + gate area and the n + source area. Aluminum (A1) gate contacts 110 and aluminum (A1) source contacts 111 are formed on the outermost element region 120 . The connection region 112 between the gate contact 110 and each gate electrode 108 is indicated by an upper right slash, and the connection portion between the source contact 111 and each source 109 is indicated by a lower left slash. As shown in FIG. 21(B), an oxide film 114 is formed on the epitaxial layer 102, and a gate contact 11 is provided on the oxide film 114. As shown in FIG. Also, although not shown, on the oxide film 114, the source contact 111 is also formed. In the above contact structure, the breakdown voltage between the gate and drain regions is about 200-300V although it depends on the thickness and quality of the oxide layer below each Al contact.

并且,由一个元件区域构成SIT。因为,漏电流与整个源长成比例,所以通过增加元件区120的面积可增加整个源长,实现源电流的增加。但是,当增加元件区120的面积时,会增加源和栅区的电阻和电感;特别在微波波段使用SIT,电阻和电感大大地影响器件的运作条件。因此,对于增加元件区的面积受到一定限制。Also, the SIT is constituted by one element region. Because the leakage current is proportional to the entire source length, the entire source length can be increased by increasing the area of the device region 120 to achieve an increase in the source current. However, when the area of the device region 120 is increased, the resistance and inductance of the source and gate regions will be increased; especially when SIT is used in the microwave band, the resistance and inductance greatly affect the operating conditions of the device. Therefore, there is a certain limit to increasing the area of the element region.

本发明的一个目的是提供一种凹栅或侧栅型SIT,它有高击穿电压的栅-漏结,并且改善了高频特性。An object of the present invention is to provide a recess gate or side gate type SIT which has a high breakdown voltage gate-drain junction and which has improved high frequency characteristics.

本发明另一个目的是提供具有大输出功率特性的高频凹栅或侧栅型SIT。Another object of the present invention is to provide a high-frequency concave-gate or side-gate type SIT having a large output power characteristic.

本发明又一个目的是提供一种凹栅或侧栅型SIT,能减少栅-漏和栅-源寄生电容。Another object of the present invention is to provide a recess gate or side gate type SIT, which can reduce gate-drain and gate-source parasitic capacitance.

本发明再一个目的是提供一种凹栅或侧栅型SIT,它允许通过大电流和减少电感。Still another object of the present invention is to provide a recess gate or side gate type SIT which allows a large current to pass and reduces inductance.

利用下述结构,可以实现本发明的目的和优点。The objects and advantages of the present invention can be achieved by the structure described below.

按照本发明的一个方案提供一个凹栅或侧栅型静态感应晶体管,它包括,第1导电类型的漏区,设置在漏区上面的具有第1导电类型的沟道区,许多槽每一个槽都形成在沟道区中,第1导电类型的许多源区,每一个都设置在沟道区中,以便被设置在各槽之间,第2导电类型的许多栅区,每一个都设置在各槽的底部,相互平行设置的栅区和源区,第2导电类型的设置在沟道区中的保护环,以便围绕栅区。在这样的结构中,保护环设置成使最外面栅区在纵向方向分别与保护环的一侧重叠,并且,每一栅区在其两边和保护环相耦连。According to a scheme of the present invention, a concave gate or side gate type static induction transistor is provided, which includes a drain region of the first conductivity type, a channel region with the first conductivity type arranged on the drain region, and a plurality of grooves for each groove are all formed in the channel region, a plurality of source regions of the first conductivity type are each arranged in the channel region so as to be arranged between the grooves, and a plurality of gate regions of the second conductivity type are each arranged in the The bottom of each groove, the gate region and the source region arranged parallel to each other, and the guard ring of the second conductivity type arranged in the channel region so as to surround the gate region. In such a structure, the guard ring is arranged such that the outermost gate regions respectively overlap one side of the guard ring in the longitudinal direction, and each gate region is coupled to the guard ring at both sides thereof.

按照本发明的另一方案,仅在保护环区设置栅和源电极以便相互对置。According to another aspect of the present invention, the gate and source electrodes are arranged so as to face each other only in the guard ring region.

在本申请所附权利要求中,将叙述本发明新颖和有区别的特征。参考附图的以下叙述,可以更好的理解本发明本身和发明的目的和优点。The novel and distinctive features of the invention are set forth in the claims appended to this application. The invention itself, together with objects and advantages thereof, may be better understood with reference to the following description of the accompanying drawings.

图1(A)是简略表示本发明SIT第1实施例的平面图;Fig. 1 (A) is the plan view that schematically represents the first embodiment of SIT of the present invention;

图1(B)是由圆包围的图1(A)部分的部分扩大的视图;Figure 1(B) is a partially enlarged view of the part of Figure 1(A) surrounded by a circle;

图2是图1(B)沿线II-II′剖开的剖视图;Fig. 2 is a sectional view taken along line II-II' of Fig. 1(B);

图3是表示宽度L1和栅区及漏区之间击穿电压之间关系的曲线图;3 is a graph showing the relationship between the width L1 and the breakdown voltage between the gate region and the drain region;

图4是表示SITS功率增益的频率特性的曲线图;FIG. 4 is a graph showing frequency characteristics of SITS power gain;

图5是简略表示按照本发明的SIT第2实施例的剖视图;Fig. 5 is a sectional view schematically showing the second embodiment of the SIT according to the present invention;

图6是简略表示按照本发明SIT第3实施例的剖视图;Fig. 6 is a sectional view schematically showing the third embodiment of the SIT according to the present invention;

图7到图12是表示按本发明制造SIT工艺的剖视图;7 to 12 are sectional views showing a process for manufacturing a SIT according to the present invention;

图13是简略表示按本发明的SIT第4实施例的平面图;Fig. 13 is a plan view schematically showing the fourth embodiment of the SIT according to the present invention;

图14是图13沿线IVX-IVX′剖开的剖视图;Fig. 14 is a sectional view taken along line IVX-IVX' of Fig. 13;

图15(A)是图13沿线XVA-XVA′剖开的剖视图;Fig. 15 (A) is a sectional view taken along the line XVA-XVA' of Fig. 13;

图15(B)是图13沿XVB-XVB′剖开的剖视图;Fig. 15 (B) is a cross-sectional view taken along XVB-XVB' of Fig. 13;

图16(A)是当接触点延伸到沟道区表面的剖分剖视图;Fig. 16(A) is a cutaway sectional view when the contact point extends to the surface of the channel region;

图16(B)是当接触点延伸到浮置区的部分剖视图;Figure 16(B) is a partial cross-sectional view when the contact point extends to the floating region;

图17是SIT的剖视图,其有作为切割区的n+区;Figure 17 is a cross-sectional view of a SIT with an n + region as a cutting region;

图18是简略表示按照本发明具有两个元件区第5实施例的平面图;Fig. 18 is a plan view schematically showing a fifth embodiment having two element regions according to the present invention;

图19是简略表示具有4个元件区的SIT平面图;Fig. 19 is a schematic plan view of a SIT with four element areas;

图20(A)到(C)是简略表示公知SITS的剖视图;Fig. 20 (A) to (C) is the sectional view that schematically shows known SITS;

图21(A)是简略表示公知SIT的平面图;FIG. 21(A) is a plan view schematically showing a known SIT;

图21(B)是图21(A)沿XXI-XXI′剖开的剖视图。Fig. 21(B) is a sectional view taken along XXI-XXI' of Fig. 21(A).

下面,参照附图,叙述本发明的实施例。Embodiments of the present invention will be described below with reference to the drawings.

首先,叙述本发明第1实施例。First, the first embodiment of the present invention will be described.

如图1(A)所示,凹栅型SIT包括许多伸长的P+栅区16(包含16和16b),许多伸长的n+源区18,围绕P+栅区16(由虚线包围的部分)象带子一样的P+保护环区13。如此设置P+栅区16和n+源区18,使其基本上和P+保护环区13的长边相互垂直,并且与保护环区13的短边相互平行。As shown in Figure 1 (A), the concave gate type SIT includes many elongated P + gate regions 16 (including 16 and 16b), many elongated n + source regions 18, surrounding the P + gate region 16 (surrounded by dotted lines part) P + guard ring region 13 like a belt. The P + gate region 16 and the n + source region 18 are arranged such that they are substantially perpendicular to the long sides of the P + guard ring region 13 and parallel to the short sides of the guard ring region 13 .

如图1(B)所示,设置在最外(最左)边的P+栅区16a在纵方向和P+保护环区13相连,设置在n+源区18之间的每一个P+栅区16b在一边缘或末端和P+保护环区13相连。把P+保护环区13的拐角弄圆,以便减轻电场强度。并且,为防止栅-源击穿电压BVgs降低,要求设置的每个n+源区18满足L2≥Wgs。在图中,L1表示P+保护环区13的宽度,L2表示n+源区18的边缘和P+保护环区13之间的距离,Wgs表示n源区18和P+栅区16之间的距离。As shown in FIG. 1(B), the P + gate region 16a disposed on the outermost (leftmost) side is connected to the P + guard ring region 13 in the longitudinal direction, and each P + gate region 16a disposed between the n + source regions 18 Gate region 16b is connected to P + guard ring region 13 at an edge or end. The corners of the P + guard ring region 13 are rounded to reduce the electric field intensity. Moreover, in order to prevent the gate-source breakdown voltage BV gs from decreasing, each n + source region 18 is required to satisfy L 2 ≥W gs . In the figure, L1 represents the width of the P + guard ring region 13, L2 represents the distance between the edge of the n + source region 18 and the P + guard ring region 13, W gs represents the n source region 18 and the P + gate region 16 distances between.

下面,参照图2更详细地叙述凹栅型SIT,其中图2是沿图1(B)线II-II′剖开的剖视图。凹栅型SIT包括n+漏区(n+衬底)11,n外延层12,它是设置在n+漏区11上面的高阻沟道区,槽14a和14b形成在n外延层12,经缘膜15形成在n外延层12上,P+栅区16a和16b形成在槽14a和14b的底部,P+保护环区13形成在n延层12中,以便和P+栅区16a的外围部分相连,设置在n外延层12的n+源区18,分别设置在P+栅区16和n+源区18的栅电极19和源电极20,设置在n+漏区11上面的漏电极21。可以利用SiO2膜,SiN膜,PSG膜或这些复合膜作为绝缘膜15。Next, the recess gate type SIT will be described in more detail with reference to FIG. 2, which is a sectional view taken along line II-II' of FIG. 1(B). The concave gate type SIT includes n + drain region (n + substrate) 11, n epitaxial layer 12, which is a high-resistance channel region arranged on n + drain region 11, grooves 14a and 14b are formed in n epitaxial layer 12, The edge film 15 is formed on the n epitaxial layer 12, the P + gate regions 16a and 16b are formed at the bottom of the grooves 14a and 14b, and the P + guard ring region 13 is formed in the n epitaxial layer 12 so as to be compatible with the P + gate region 16a. The peripheral part is connected, and the n + source region 18 set on the n epitaxial layer 12, the gate electrode 19 and the source electrode 20 respectively set on the P + gate region 16 and the n + source region 18, and the drain electrode 20 set on the n + drain region 11 Pole 21. As the insulating film 15, a SiO 2 film, a SiN film, a PSG film, or a composite film of these can be utilized.

在图2中,W1表示n外延层12的厚度,W2表示P+栅区16和n+漏区11之间的距离,W3表示P+保护环区13和n+漏区11之间的距离,Xj表示P+保护环区13的扩散深度,Rj表示P+保护环区13的曲率半径,R是大约Xj的80%。In FIG. 2, W1 represents the thickness of the n epitaxial layer 12, W2 represents the distance between the P + gate region 16 and the n + drain region 11, and W3 represents the distance between the P + guard ring region 13 and the n + drain region 11 Xj represents the diffusion depth of the P + guard ring region 13, Rj represents the curvature radius of the P + guard ring region 13, and R is about 80% of Xj.

例如,假定W1是9μm,槽14的深度是1-1.5μm,P+栅区16的扩散深度是大约0.5μm。对于常规器件,没有P+保护环区,BVgd是大约50-60V。相反,对于本发明的器件,设置P+保护环区13,它的L1为8-13μm,Xj大约为2μm,则BVgd变成120-140V;是常规器件的有关参数数值的两倍以上。For example, assuming that W 1 is 9 μm, the depth of groove 14 is 1-1.5 μm, and the diffusion depth of P + gate region 16 is about 0.5 μm. For a conventional device, without the P + guard ring region, BV gd is about 50-60V. On the contrary, for the device of the present invention, the P + guard ring region 13 is set, its L1 is 8-13 μm, and Xj is about 2 μm, then BV gd becomes 120-140V; it is more than twice the relevant parameter value of the conventional device .

在上述结构中,认为n+漏区11和n外延层12之间的过渡区厚度W2是大约7μm。在此情况,由p+栅区16的平面结区确定的理论击穿电压是大约156V。按照本发明具有P+保护环13的结构能提供接近理论击穿电压90%的数值。In the above structure, the transition region thickness W2 between n + drain region 11 and n epitaxial layer 12 is considered to be about 7 µm. In this case, the theoretical breakdown voltage determined by the planar junction region of p + gate region 16 is about 156V. The structure according to the invention with the P + guard ring 13 can provide values close to 90% of the theoretical breakdown voltage.

其次,叙述P+保护环区13的的宽度L1。在SIT中设置P+保护环区13,则在P+保护环13和n+漏区11之间产生寄生电容Cgd′,除非Cg与P+栅区16和n+漏区11之间电容Cgd充分的小,否则会降低高频特性,由此而减少功率增益。所以必须减少Cgd′。并要尽可能的减少L1。但是,如果L1太短,因为由设置在P+保护环区13外围的柱形结区决定击穿电压因而降低击穿电压BVgd。因此需要通过考虑L1和BVgd之间关系,来确定P+保护环区13的宽度L1Next, the width L 1 of the P + guard ring region 13 is described. If the P + guard ring region 13 is set in the SIT, a parasitic capacitance C gd ' will be generated between the P + guard ring 13 and the n + drain region 11, unless C g is between the P + gate region 16 and the n + drain region 11 The capacitor C gd is sufficiently small, otherwise the high-frequency characteristics will be degraded, thereby reducing the power gain. So C gd ' must be reduced. And to reduce L 1 as much as possible. However, if L 1 is too short, the breakdown voltage BV gd is lowered because the breakdown voltage is determined by the columnar junction region disposed on the periphery of the P + guard ring region 13 . Therefore, it is necessary to determine the width L 1 of the P + guard ring region 13 by considering the relationship between L 1 and BV gd .

保护环区13的杂质浓度可以等于或小于P+栅区16a和16b的杂质浓度。如果保护环区13的杂质浓度小于P+栅区16a、16b的杂质浓度,则耗尽层延伸到P+保护环区13,并进一步增加击穿电压和减少寄生电容。The impurity concentration of guard ring region 13 may be equal to or less than the impurity concentration of P + gate regions 16a and 16b. If the impurity concentration of the guard ring region 13 is lower than that of the P + gate regions 16a, 16b, the depletion layer extends to the P + guard ring region 13, further increasing breakdown voltage and reducing parasitic capacitance.

虽然,在图1(A)中没有表示栅和源接触点,但是,和许多伸长的P+栅区16的一个边缘相连的栅接触点,以及和许多伸长的n+源区1的一个边缘相连的源接触点是利用绝缘膜而被设置在有P+保护环区13的n外延层12上面,这样使它们彼此相对。Though, in Fig. 1 (A), do not represent grid and source contact point, but, the gate contact point that is connected with an edge of many elongated P + gate regions 16, and the n + source region 1 of many elongate An edge-connected source contact is provided on the n epitaxial layer 12 with the P + guard ring region 13 by using an insulating film so that they are opposed to each other.

图3表示SIT中P+保护环宽度L1和栅-漏击穿电压BVgd之间的关系,该SIT具有W1为9μm,槽14深为1-1.5μm,规定P+栅16扩散深度为大约0.5μm,Xj为2μm。按照图3,当L1是大约8μm以上时,则BVgd达到饱和。当L1是8μm以上时,耗尽层延伸到漏区11,并且超过由P+栅区16到n+漏区11的距离W2(大约7-7.5μm),由此,降低表面电场强度。这意味着在器件中由P+栅区16的平面结部分确定击穿电压BVgd。因此,为获得预定击穿电压和同时减少寄生电容Cgd′要求P+保护环13的宽度L1几乎等于或稍大于W2Figure 3 shows the relationship between the P + guard ring width L1 and the gate-drain breakdown voltage BV gd in a SIT with a W1 of 9 μm and a groove 14 depth of 1-1.5 μm, specifying the P + gate 16 diffusion depth is about 0.5 μm, and Xj is 2 μm. According to FIG. 3 , when L 1 is about 8 μm or more, BV gd is saturated. When L 1 is above 8 μm, the depletion layer extends to the drain region 11, and exceeds the distance W 2 (approximately 7-7.5 μm) from the P + gate region 16 to the n + drain region 11, thereby reducing the surface electric field intensity . This means that the breakdown voltage BVgd is determined by the planar junction portion of the P + gate region 16 in the device. Therefore, in order to obtain a predetermined breakdown voltage and simultaneously reduce the parasitic capacitance C gd ′, it is required that the width L 1 of the P + guard ring 13 is almost equal to or slightly larger than W 2 .

图4表示功率增益和频率之间的关系,它是通过测量凹栅型SIT的S参数算出的,SIT具有并联的100个伸长的源区(每个源长120nμm总源长1.2cm)。具有L1规定为大的8μm的本发明SIT和没有保护环结构的常规SIT比较如下所示。偏置条件如下所示:(本发明的SIT有P+保护环,具有大的BVgd,Vds是为50V,是常规SIT的两倍)   偏置条件   Vds(V)   Id(mA)   Vgs(V)   本发明SIT     50     50     -3.17   常规SIT     25     50     -4.45 Figure 4 shows the relationship between power gain and frequency, which is calculated by measuring the S-parameters of a concave-grid SIT with 100 elongated source regions in parallel (each source length is 120nμm and the total source length is 1.2cm). The comparison between the SIT of the present invention having L 1 defined as large at 8 µm and the conventional SIT without the guard ring structure is shown below. The bias conditions are as follows: (the SIT of the present invention has a P + guard ring, has a large BV gd , and V ds is 50V, which is twice that of the conventional SIT) bias condition Vds(V) Id(mA) Vgs(V) SIT of the present invention 50 50 -3.17 Conventional SIT 25 50 -4.45

如图4所示,对于最稳定的增益而言,由于Cgd′,本发明SIT中减少增益0.5db。但是,对于最有用的增益,本发明的SIT的功率增益几乎与常规SIT的功率增益相等,在某些频率还大于常规SIT的功率增益,这是因为除了Cgd和Cgd′外,还受电感的影响。按照本发明的SIT击穿电压可能增加到常规SIT击穿电压的2倍以上,而不降低频率特性。这意味着,SIT的许可的直流(DC)输入可能被加倍,因此,和具有相同源长的SIT比较,使本发明输出功率加倍。As shown in Fig. 4, for the most stable gain, the gain is reduced by 0.5db in the inventive SIT due to Cgd '. However, for the most useful gain, the power gain of the SIT of the present invention is almost equal to that of the conventional SIT, and at some frequencies is greater than that of the conventional SIT, because in addition to C gd and C gd ', also affected by The effect of inductance. The SIT breakdown voltage according to the present invention can be increased to more than 2 times the conventional SIT breakdown voltage without degrading the frequency characteristics. This means that the permitted direct current (DC) input of the SIT may be doubled, thus doubling the output power of the invention compared to a SIT with the same source length.

其次,参看图5,叙述本发明的第2实施例。用相同标号表示与图2类似的部分。P+浮置区22具有类似于P+保护环区13的杂质浓度,P+保护环区13形成在n外延层12中,使P+浮置区22环绕P+保护环区13。可以2倍或3倍的设置P+浮置区22,以便获得较高的击穿电压。Next, referring to Fig. 5, a second embodiment of the present invention will be described. Parts similar to those in Fig. 2 are denoted by the same reference numerals. P + floating region 22 has an impurity concentration similar to that of P + guard ring region 13 formed in n epitaxial layer 12 such that P + floating region 22 surrounds P + guard ring region 13 . The P + floating region 22 can be set 2 times or 3 times, so as to obtain a higher breakdown voltage.

图6表示本发明的第3实施例,其中,在P+保护环区13的周围设置n+区23。它防止从保护环区13延伸的耗尽层过度的延伸、并且被用作沿线A-A′的切割区。当按照n+区23,把晶片切成小块时,可能防止不想产生和增加的漏电流。最好,n+区23的扩散深度,至少是比P+保护环区13深,并且可以达到n+漏区11。P+浮置区22可以设置在保护环区13的周围,在其周围可以提供n+区23。FIG. 6 shows a third embodiment of the present invention in which an n + region 23 is provided around a p + guard ring region 13 . It prevents excessive extension of the depletion layer extending from guard ring region 13 and is used as a cutting region along line AA'. When the wafer is diced according to the n + region 23, it is possible to prevent unintended and increased leakage current. Preferably, the diffusion depth of the n + region 23 is at least deeper than that of the P + guard ring region 13 and can reach the n + drain region 11 . P + floating region 22 may be provided around guard ring region 13, and n + region 23 may be provided therearound.

参照图7到图12,叙述本发明的一种制造SIT的方法,它表示沿图1(B)II-II′线剖开的剖视图。Referring to Fig. 7 to Fig. 12, describe a kind of method of manufacturing SIT of the present invention, it shows the sectional view along line II-II' of Fig. 1 (B).

首先,制备作为漏区的n+衬底11,其是(100)或(111)平面,杂质浓度大约为1×1018到1×1019cm-3,下文将其称为n+漏区。利用SiCl4和H2,通过汽相生长方法,在n+漏区11上面、生长高阻n-型外延层12。n外延层12的杂质浓度是1×1013cm-3或更小或1×1013到1×1015cm-3。为了获得恰好夹断特性,邻接衬底11的n外延层1下部的杂质浓度是1×1013cm-3,从其表面向下2-3μm的n外延层上部杂质浓度是5×1014到1×1015cm-3。按照设计,n外延层12具有均匀或非均匀杂质浓度分布。利用SiO2等(未表示)作为掩模(图7通过离子注入等方法,在n外延层12中形成P+保护环区13,其杂质浓度为1×1017到1×1020cm-3First, prepare an n + substrate 11 as a drain region, which is a (100) or (111) plane, and has an impurity concentration of approximately 1×10 18 to 1×10 19 cm −3 , which is hereinafter referred to as an n + drain region . A high-resistance n-type epitaxial layer 12 is grown on the n + drain region 11 by using SiCl 4 and H 2 by a vapor phase growth method. The impurity concentration of n epitaxial layer 12 is 1×10 13 cm −3 or less or 1×10 13 to 1×10 15 cm −3 . In order to obtain just pinch-off characteristics, the impurity concentration in the lower part of the n-epitaxial layer 1 adjacent to the substrate 11 is 1×10 13 cm −3 , and the impurity concentration in the upper part of the n-epitaxial layer 2-3 μm down from the surface is 5×10 14 to 1×10 15 cm -3 . By design, n-epitaxial layer 12 has a uniform or non-uniform impurity concentration distribution. Using SiO 2 etc. (not shown) as a mask (Fig. 7, form a P + guard ring region 13 in the n epitaxial layer 12 by ion implantation and other methods, and its impurity concentration is 1×10 17 to 1×10 20 cm -3 .

其次,利用SiO2膜(未表示)作为掩模,通过RIE(反应离子腐蚀方法,在n外延层12中,形成许多作为凹栅的伸长槽14a和14b。形成最外边槽14a,在纵向部分地重叠P+保护环区13,形成槽14b,在两边(未表示)重叠P+保护环区13。槽14a和14b分别是2μm和1μm宽,1-1.5μm深。槽14a和槽14b间隔3-7μm,RIE利用SF6和O2气混合等离子体(图8)。Next, utilize SiO 2 film (not shown) as mask, by RIE (reactive ion etching method, in n epitaxial layer 12, form many elongated grooves 14a and 14b as concave grid. Form outermost edge groove 14a, in vertical direction Partially overlap the P + guard ring region 13 to form a groove 14b, overlapping the P + guard ring region 13 on both sides (not shown). The grooves 14a and 14b are 2 μm and 1 μm wide and 1-1.5 μm deep, respectively. Groove 14a and groove 14b With an interval of 3-7 μm, RIE utilizes a mixed plasma of SF6 and O2 gas (Fig. 8).

然后,通过在水蒸气中氧化n外延层12,形成绝缘膜15,例如厚度为大约0.5-1μm的厚氧化膜。RIE利用CF4或CF4和CHF3混合气体选择地腐蚀绝缘膜15,以从槽14a和槽14b底部暴露出n外延层12。接着,对露出的槽14a和14b的底部进行硼扩散和离子注入,以便提供P+栅区16a和16b,其杂质浓度为1×1018到1×1020cm-3,在此工艺中,P+栅区16a和P+保护环区13相连。同样,在两边(未表示)把P+栅区16b和P+保护环区13相连。P+栅区16的扩散深度大约是0.5μm(图9)。Then, by oxidizing the n-epitaxial layer 12 in water vapor, an insulating film 15 is formed, for example, a thick oxide film having a thickness of about 0.5-1 [mu]m. RIE uses CF 4 or a mixed gas of CF 4 and CHF 3 to selectively etch the insulating film 15 to expose the n epitaxial layer 12 from the bottom of the groove 14 a and the groove 14 b. Next, boron diffusion and ion implantation are performed on the exposed bottoms of trenches 14a and 14b to provide P + gate regions 16a and 16b with an impurity concentration of 1×10 18 to 1×10 20 cm -3 . In this process, The P + gate region 16a is connected to the P + guard ring region 13 . Likewise, the P + gate region 16b is connected to the P + guard ring region 13 on both sides (not shown). The diffusion depth of the P + gate region 16 is about 0.5 μm (FIG. 9).

其次,在衬底表面形成光致抗蚀剂等材料的掩模图形,利用RIE等方法,选择地除去绝缘膜15,以便露出n型外延层12(图10)。把磷或砷离子注入到延伸的n外延层12,以便在其中提供n+源区18。此后,除去掩模图形17。如果把SiO2等作为掩模图形17,也可以通过扩散多晶硅层所含的n-型杂质形成n+源区18,(图11),以后,分别在P+栅区16,n+源区18,n+漏区11形成栅电极19,源电极20,和漏电极21,(图12)。Next, a mask pattern of a material such as photoresist is formed on the surface of the substrate, and the insulating film 15 is selectively removed by using a method such as RIE to expose the n-type epitaxial layer 12 ( FIG. 10 ). Phosphorous or arsenic ions are implanted into extended n epitaxial layer 12 to provide n + source regions 18 therein. Thereafter, the mask pattern 17 is removed. If SiO 2 etc. are used as the mask pattern 17, the n + source region 18 can also be formed by diffusing the n-type impurities contained in the polysilicon layer, (Fig. 11). 18, n + drain region 11 forms gate electrode 19, source electrode 20, and drain electrode 21, (FIG. 12).

其次,参照附图13-17,叙述本发明第4实施例。Next, a fourth embodiment of the present invention will be described with reference to Figs. 13-17.

如图13所示,凹栅型SIT包括许多伸长的P+栅区37(包括37a和37b),许多伸长的源区39,矩形P+保护环区33,它包围P+栅区37(在图中由虚线包围),位于P+保护环区33外围的P+浮置区34,栅电极布线层40设置在P+栅区37上面,并在P+保护环区33上面相互连接,源电极布线层41设置在n+源区39上面,在P+保护环区33上面互连,栅接点(焊点)43与栅电极布线层40相连,源接触点(焊点)44与源电极布线层41相连。在这种情况,栅和源接触点43和44被设置在P+保护环区33。As shown in Figure 13, the concave gate type SIT includes many elongated P + gate regions 37 (including 37a and 37b), many elongated source regions 39, and a rectangular P + guard ring region 33, which surrounds the P + gate region 37 (surrounded by dotted lines in the figure), the P + floating region 34 located on the periphery of the P + guard ring region 33, the gate electrode wiring layer 40 is arranged on the P + gate region 37, and is connected to each other on the P + guard ring region 33 , the source electrode wiring layer 41 is arranged on the n + source region 39, interconnected on the P + guard ring region 33, the gate contact point (soldering point) 43 is connected to the gate electrode wiring layer 40, and the source contact point (soldering point) 44 is connected to the The source electrode wiring layer 41 is connected. In this case, gate and source contacts 43 and 44 are provided in the P + guard ring region 33 .

由图13显而易见,栅电极布线层40由左斜线表示,源电极布线层41由右斜线表示。例如,利用掺硼多晶硅作为栅和源电极布线层40和41,利用如Al或Al-Si金属作栅和源接点43和44。As apparent from FIG. 13 , the gate electrode wiring layer 40 is indicated by left oblique lines, and the source electrode wiring layer 41 is indicated by right oblique lines. For example, boron-doped polysilicon is used for the gate and source electrode wiring layers 40 and 41, and metal such as Al or Al-Si is used for the gate and source contacts 43 and 44.

平行地交替设置P+栅区37和n+源区39。设置在最外边的P+栅区37a在纵向被连到P+保护环区33,夹在n+源区39之间的每一P+栅区37b在两边与P+保护环33相连。把P+保护环区33的拐角弄圆,以便降低电场强度,设置P+栅区37和n+源区39与P+保护环区33的相对两长边相互垂直,并与栅和源接点43及44的中心线相互对称。栅和源电极布线线层40和41具有指状电极结构。P + gate regions 37 and n + source regions 39 are alternately arranged in parallel. The P + gate region 37a disposed on the outermost side is connected to the P + guard ring region 33 in the longitudinal direction, and each P + gate region 37b sandwiched between the n + source regions 39 is connected to the P + guard ring 33 on both sides. The corners of the P + guard ring region 33 are rounded so that the electric field intensity is reduced, the opposite two long sides of the P + gate region 37 and the n + source region 39 and the P + guard ring region 33 are perpendicular to each other, and are connected to the gate and the source contact The centerlines of 43 and 44 are symmetrical to each other. The gate and source electrode wiring layers 40 and 41 have a finger electrode structure.

参照图14叙述凹栅型SIT的剖面,它是沿图13线IVX-IVX′剖开的剖视图。凹栅型SIT包括n+漏区(n+衬底)31,设置在n+漏区31上面的高阻沟道区中的n外延层32,在n外延层32中形成的槽35a和35在n外延层32上形成绝缘膜36,从槽35a和35b的底部在n外延层32上形成P+栅区37a和37b,在n外延层32中形成P+保护环区33,以便在纵向使其和P+栅区37的外围部分相连,在n外延层32中形成P+浮置区34,在n外延层32上设置源区39,在P+栅区37和n+源区39上分别淀积栅和源电极布线层40和41,在n+漏区31上面设置漏电极42。把SiO2膜,SiN膜,PSG膜,聚酰胺膜,或这些复合膜用作绝缘膜36。The cross section of the recess gate type SIT will be described with reference to FIG. 14, which is a cross section taken along line IVX-IVX' in FIG. The recessed gate type SIT includes an n + drain region (n + substrate) 31, an n epitaxial layer 32 disposed in a high-resistance channel region above the n + drain region 31, grooves 35a and 35 formed in the n epitaxial layer 32 An insulating film 36 is formed on the n epitaxial layer 32, P + gate regions 37a and 37b are formed on the n epitaxial layer 32 from the bottom of the grooves 35a and 35b, and a P + guard ring region 33 is formed in the n epitaxial layer 32, so that in the vertical direction Make it connected to the peripheral part of the P + gate region 37, form the P + floating region 34 in the n epitaxial layer 32, set the source region 39 on the n epitaxial layer 32, and set the P + gate region 37 and the n + source region 39 Gate and source electrode wiring layers 40 and 41 are respectively deposited on it, and a drain electrode 42 is provided on the n + drain region 31 . As the insulating film 36, a SiO2 film, a SiN film, a PSG film, a polyamide film, or a composite film of these is used.

如图15(A)所示,P+栅区37b和P+保护区33相互连接。每一栅电极布线层40被设置在P+栅区37b,并通过绝缘膜36延伸到P+保护环区33,栅接触点43被设置在P+保护环区33上面的栅电极布线层40上面。如图15(B)所示,设置在n+源区39上的每一源电极布线层41,通过绝缘膜36延伸到P+保护环区33,源接点44形成在P+保护环区33上面的源电极布线41上面。As shown in FIG. 15(A), the P + gate region 37b and the P + guard region 33 are connected to each other. Each gate electrode wiring layer 40 is arranged on the P + gate region 37b, and extends to the P + guard ring region 33 through the insulating film 36, and the gate contact point 43 is arranged on the gate electrode wiring layer 40 above the P + guard ring region 33 above. As shown in FIG. 15(B), each source electrode wiring layer 41 provided on the n + source region 39 extends to the P + guard ring region 33 through the insulating film 36, and the source contact 44 is formed in the P + guard ring region 33 above the source electrode wiring 41 .

如上所述,把栅和源接点43和44只淀积在P+保护环33上。如图16(A)所示,如果栅电极接点43′延伸到P+保护环区33和P+浮置区34之间的部分,则在圆部分A降低击穿电压。如图16(B)所示,如果接点43″达到或者超过P+浮置区34,则减少栅-漏击穿电压BVgd,并增加栅-漏电容Cgd,因此,减少高频区的功率增益。此外,产生包括P+保护环区33,n外延层32和P+浮置区34的寄生MOS晶体管。因此,如果栅漏击穿电压BVgd,例如是大约600V,它随时间减少到大约300V。因此,需要只在P+保护环区33上面设置栅和源接触点43。Gate and source contacts 43 and 44 are deposited on P + guard ring 33 only, as described above. As shown in FIG. 16(A), if the gate electrode contact 43' extends to the portion between the P + guard ring region 33 and the P + floating region 34, the breakdown voltage is lowered at the circle portion A. As shown in FIG. 16(B), if the contact point 43″ reaches or exceeds the P + floating region 34, the gate-drain breakdown voltage BV gd is reduced, and the gate-drain capacitance C gd is increased, thus reducing the Power gain. In addition, a parasitic MOS transistor including P + guard ring region 33, n epitaxial layer 32 and P + floating region 34 is produced. Therefore, if the gate-drain breakdown voltage BV gd is, for example, about 600V, it decreases with time to about 300 V. Therefore, gate and source contacts 43 need to be provided only on the P + guard ring region 33 .

而且,因为P+栅区37a最外围部分,沿纵向和P+保护区33相连,由P+栅区37的平面结部分确定栅漏击穿电压BVgd,可使BVgd增强到几乎是理论击穿电压。但是,如果栅源接触点43和44位于P+保护环区33的最外边,如上所述,将降低击穿电压。因此,如想使SIT击穿电压变高,则要设置P+保护环区33,并且把栅和源接触点43和44只设置在P+保护环区33上面。Moreover, because the outermost part of the P + gate region 37a is connected to the P + guard region 33 in the vertical direction, the gate-to-drain breakdown voltage BV gd is determined by the planar junction part of the P + gate region 37, which can enhance the BV gd to almost a theoretical breakdown voltage. However, if the gate-source contacts 43 and 44 are located on the outermost edge of the P + guard ring region 33, as described above, the breakdown voltage will be reduced. Therefore, if it is desired to increase the breakdown voltage of the SIT, the P + guard ring region 33 must be provided, and the gate and source contacts 43 and 44 are only provided on the P + guard ring region 33 .

例如,当外延层32是35-55μm厚,槽35是1-1.5μm深,相互间距离是7-10μm,P+保护环区33在掩模层是30-50μm宽,P+保护环区3的扩散深度是大约5μm,则凹栅型SIT具有大约300-600V的栅-漏击穿电压BVgd,在10MHZ时具有功率增益20-25db,在100MHZ时具有功率增益10-15db。For example, when the epitaxial layer 32 is 35-55 μm thick, the grooves 35 are 1-1.5 μm deep, and the distance between them is 7-10 μm, the P + guard ring region 33 in the mask layer is 30-50 μm wide, and the P + guard ring region 3 diffusion depth is about 5 μm, the concave gate SIT has a gate-drain breakdown voltage BV gd of about 300-600V, a power gain of 20-25db at 10MHZ, and a power gain of 10-15db at 100MHZ.

并且,如图17所示,可以在P+浮置区34的外围设置n+区45。当沿线B-B′切割晶片时,可能防止产生和增加漏电流。最好,至少使n+区扩散深度比P+保护环区33的深度更深。Also, as shown in FIG. 17 , n + region 45 may be provided on the periphery of P + floating region 34 . When the wafer is diced along the line BB', it is possible to prevent the leakage current from being generated and increased. Preferably, at least the n + region is diffused deeper than the p + guard ring region 33 depth.

其次,叙述本发明第5实施例。Next, a fifth embodiment of the present invention will be described.

图18表示SIT,它包括并联的两个单元5a和50b,每个单元有栅和源等,与图13所示相同。图18中单元50a和50b的细节与图13中的情况相同,并且被省略,连续设置P+保护环区33,以便限定矩形单元50a和50b,在单元50a和50b之间形成与栅区两边相连的P+保护环区331。FIG. 18 shows a SIT, which includes two units 5a and 50b connected in parallel, each unit having a gate and a source, etc., as shown in FIG. 13 . The details of the cells 50a and 50b in FIG. 18 are the same as those in FIG. 13 and are omitted. The P + guard ring region 33 is continuously arranged so as to define the rectangular cells 50a and 50b. The connected P + guard ring region 331 .

单元50a的源接点44a和单元50b的源电极接点44b,几乎设置在P+保护环区33两外部长边的中心。和单元50a及50b的栅区相连的栅接触点43与源接触点44a和44b排在一直线上(对准),并且被设置在共公的P+保护环区331上面。如图18所示,在每个单元中,P+栅区和n+源区与P+保护环区33的相对长边相互垂直,并相对于栅和源接触点43,44a,44b的中心线是对称的。对于设置栅和源接触点43,44a,44b的P+保护环区33的面积和他的其它部分相比是被增加了The source contact 44a of the cell 50a and the source electrode contact 44b of the cell 50b are located almost in the center of the two outer long sides of the P + guard ring region 33 . Gate contact 43, which is connected to the gate regions of cells 50a and 50b, is in-line (aligned) with source contacts 44a and 44b, and is disposed over common P + guard ring region 331. As shown in FIG. 18, in each cell, the opposite long sides of the P+ gate region and the n + source region and the P + guard ring region 33 are perpendicular to each other, and relative to the center line of the gate and source contact points 43, 44a, 44b is symmetrical. The area of the P + guard ring region 33 for setting the gate and source contacts 43, 44a, 44b is increased compared to its other parts

图19表示包括4个并联单元50a-50d的SIT。在这种情况,如图18所示,设置一矩形P+保护环区33,以便限定单元50a到50d。只在P+保护环区33上面交替地设置源接触点44和栅接触点43。Figure 19 shows a SIT comprising 4 parallel units 50a-50d. In this case, as shown in FIG. 18, a rectangular P + guard ring region 33 is provided so as to define cells 50a to 50d. Source contact 44 and gate contact 43 are provided alternately only on P + guard ring region 33 .

于是,在具有公共部分的P+栅保护区33上面设置栅和源接触点43和44,则容易并联大量单元50。考虑电流容量和电阻等,在每个保护环区可以设置两个或更多的接触点。在接触点下面的P+保护环区33具有要求的结构。由于沟道具有高阻,则在单元内容易被吸收(digestion)。Thus, by providing gate and source contacts 43 and 44 above the P + gate guard region 33 having a common portion, a large number of cells 50 can be easily connected in parallel. Considering the current capacity and resistance, etc., two or more contact points can be set in each guard ring area. The P + guard ring region 33 below the contact has the required structure. Since the channel has high resistance, it is easy to be absorbed in the cell (digestion).

当把SIT用在比HF频段更高的VHF或UHF时,不能忽略源和栅电感的影响。但是,包括并联几个小面积单元50的器件,和仅有一个大面积单元的器件结构相比,它可以减少不希望的电感。而且那样的器件可能一致的运作。When using SIT at VHF or UHF higher than HF band, the effect of source and gate inductance cannot be ignored. However, a device comprising several small area cells 50 in parallel can reduce undesirable inductance compared to a device structure with only one large area cell. And such devices may operate consistently.

利用与图7-12所示类似的工艺,可能制造第4和第5实施例所示的器件。Using processes similar to those shown in Figs. 7-12, it is possible to manufacture the devices shown in the fourth and fifth embodiments.

虽然,已经叙述了凹栅型SIT,但是类似的叙述也适用于侧栅型SIT。本发明不仅适用于由Si制作的SIT,而且适用于由GaAs,InP等制作的化合物半导体(制作的器件),这是不必说的。Although, the recess gate type SIT has been described, similar descriptions apply to the side gate type SIT. Needless to say, the present invention is applicable not only to SIT made of Si but also to compound semiconductors (fabricated devices) made of GaAs, InP, etc.

按照本发明,在凹栅或侧栅型SIT中,在栅区的周围,设置保护环区,由此,显著地增加栅漏结击穿电压。对于本发明的SIT,和常规的SIT相比,可以使在漏和源之间加的电压变成两倍以上,而不降低高频特性,并且提供有高输出功率的SIT。设置P+保护环区,以便与P+栅区最外边部分耦连,并且仅在P+保护环区设置栅和源接触点由此,可以改善击穿电压和提供具有优良高频特性的SIT。并且,容易提供并联的小面积单元,由此,增加整个源长度和减少电感。According to the present invention, in the recess gate or side gate type SIT, a guard ring region is provided around the gate region, thereby significantly increasing the breakdown voltage of the gate-drain junction. With the SIT of the present invention, the voltage applied between the drain and the source can be made more than twice as compared with the conventional SIT without degrading high-frequency characteristics, and a SIT with high output power is provided. The P + guard ring region is set so as to be coupled with the outermost part of the P + gate region, and the gate and source contacts are provided only in the P + guard ring region. Thus, the breakdown voltage can be improved and SIT with excellent high-frequency characteristics can be provided . Also, it is easy to provide small-area cells connected in parallel, thereby increasing the overall source length and reducing inductance.

本领域技术人员应进一步了解,前面的说明是公开器件的优选实施例,本发明可以进行各种变化和修改,但均不脱离本发明的精神实质和范围。Those skilled in the art should further understand that the foregoing descriptions are preferred embodiments of the disclosed devices, and various changes and modifications can be made in the present invention without departing from the spirit and scope of the present invention.

Claims (14)

1,一种静态感应晶体管,它包括,1. A static sensing transistor comprising, 具有第1导电类型的漏区;a drain region having a first conductivity type; 设置在所述漏区上面有所述第1导电类型的沟道区;a channel region of the first conductivity type is disposed above the drain region; 许多沟槽,每一个沟槽形成在所述的沟道区中;a plurality of trenches, each trench formed in said channel region; 许多源区,它具有所述的第1导电类型,每一源区设置在所述沟道区中,以便被设置在所述的许多槽之间;a plurality of source regions, having said first conductivity type, each source region disposed in said channel region so as to be disposed between said plurality of trenches; 许多栅区,具有第2导电类型,每一栅区设置在所述槽的底部,其中,所述许多栅区和所述许多源区相互平行设置;A plurality of gate regions having a second conductivity type, each gate region is disposed at the bottom of the groove, wherein the plurality of gate regions and the plurality of source regions are arranged parallel to each other; 保护环区,具有所述的第2导电类型,设置在所述沟道区,围绕所述许多栅区设置所述的保护环区,使所述许多栅区中的最外边栅区分别与所述保护环区的一边重叠,所述许多栅区中的每一个在两边和所述保护环区相连。A guard ring region, having the second conductivity type, is arranged in the channel region, and the guard ring region is arranged around the plurality of gate regions, so that the outermost gate regions of the plurality of gate regions are respectively connected to the plurality of gate regions. One side of the guard ring region overlaps, and each of the plurality of gate regions is connected to the guard ring region on two sides. 2,按照权利要求1的静态感应晶体管,其特征是,所述保护环的宽度等于或者大于所述许多栅区中的每一栅区与所述漏区之间的距离。2. The static induction transistor according to claim 1, wherein said guard ring has a width equal to or greater than a distance between each of said plurality of gate regions and said drain region. 3,按照权利要求1的静态感应晶体管,其特征是,在所述沟道区设置具有所述第2导电类型的浮置区,以便包围所述保护环区。3. The static induction transistor according to claim 1, wherein a floating region having said second conductivity type is provided in said channel region so as to surround said guard ring region. 4,按照权利要求1的静态感应晶体管,其特征是,在所述沟道区设置具有所述第1导电类型的半导体区,以便包围所述保护环区。4. The static induction transistor according to claim 1, wherein a semiconductor region having said first conductivity type is provided in said channel region so as to surround said guard ring region. 5,按照权利要求4的静态感应晶体管,其特征是,利用所述的半导体区作为切割区。5. The static induction transistor according to claim 4, wherein said semiconductor region is used as a cutting region. 6,按照权利要求1的静态感应晶体管,其特征是,在所述沟道区利用绝缘膜,设置具有指状结构的源和栅电极。6. The static induction transistor according to claim 1, wherein source and gate electrodes having a finger structure are provided in said channel region using an insulating film. 7,一种静态感应晶体管包括:7. A static sensing transistor comprising: 具有第1导电类型的漏区;a drain region having a first conductivity type; 在所述漏区上面设置沟道区,它具有所述的第1导电类型;disposing a channel region above said drain region, which has said first conductivity type; 许多沟槽,其中每一沟槽形成在所述沟道区中,并且具有一底部;a plurality of trenches, each of which is formed in the channel region and has a bottom; 具有所述第1导电类型的许多源区,每一源区设置在所述沟道区上面,以便被设置在所述许多槽之间,其中相互平行地设置所述的许多槽和所述的许多源区;a plurality of source regions having said first conductivity type, each source region being disposed above said channel region so as to be disposed between said plurality of grooves, wherein said plurality of grooves and said plurality of grooves are arranged parallel to each other many source regions; 许多栅区,具有第2导电类型,每一个栅区设置在所述的底部;a plurality of gate regions, having a second conductivity type, each gate region is disposed on said bottom; 设置在所述沟道区的保护环区,具有第2导电类型,设置所述的保护环区,包围所述许多栅区,使所述许多栅区中的最外边栅区,分别与所述保护环区的一边互相重叠,并且,所述许多栅区中的每一个栅区在其两边和所述的许多栅区耦连;The guard ring region disposed in the channel region has the second conductivity type, the guard ring region is arranged to surround the plurality of gate regions, so that the outermost gate regions of the plurality of gate regions are respectively connected to the One side of the guard ring region overlaps each other, and each gate region in the plurality of gate regions is coupled to the plurality of gate regions on both sides thereof; 源电极,其中每一个源电极设置在所述许多源区中的相应的一个源区上;source electrodes, wherein each source electrode is disposed on a corresponding one of the plurality of source regions; 栅电极,其中每一个栅电极设置在所述栅区中的相应一个栅区上;gate electrodes, wherein each gate electrode is disposed on a corresponding one of the gate regions; 第1和第2接触点,利用绝缘膜被设置在所述保护环区,并分别与所述源电极和所述栅电极相连。The first and second contact points are provided in the guard ring region with an insulating film, and are respectively connected to the source electrode and the gate electrode. 8,按照权利要求7的静态感应晶体管,其特征是,使所述许多源区中的每一个源区和所述许多栅区中的每一个栅区相互交叉设置。8. The static induction transistor according to claim 7, wherein each source region of said plurality of source regions and each gate region of said plurality of gate regions are arranged to cross each other. 9,按照权利要求7的静态感应晶体管,其特征是,相互相对设置所述第1和第2接触点。9. The static sensing transistor according to claim 7, wherein said first and second contact points are arranged opposite to each other. 10,按照权利要求7的静态感应晶体管,其特征是,所述许多栅区和所述许多源区,相对于连接所述第1和第2接触点的直线是对称的。10. The static sensing transistor according to claim 7, wherein said plurality of gate regions and said plurality of source regions are symmetrical with respect to a line connecting said first and second contact points. 11.一种静态感应晶体管包括:11. A static sensing transistor comprising: 具有第1导电类型的漏区;a drain region having a first conductivity type; 设置在所述漏区上面的沟道区,具有所述第1导电类型;a channel region disposed above the drain region, having the first conductivity type; 具有第2导电类型的保护环区,所述保护环区设置在所述的沟道区,以便限定由所述保护环区的公共区隔开的第1和第2区;a guard ring region having a second conductivity type disposed in said channel region so as to define first and second regions separated by a common region of said guard ring region; 许多槽,其中每一槽形成在所述第1和第2区中的所述每一区中并且有一个底部;a plurality of grooves, wherein each groove is formed in said each of said first and second regions and has a bottom; 具有所述第1导电类型的许多源区,每一源区设置在所述第1和第2区中的所述每一区上,以便被设置在所述许多槽之间,其中,所述许多槽和所述许多源区相互平行地设置;a plurality of source regions having said first conductivity type, each source region being disposed on said each of said first and second regions so as to be disposed between said plurality of grooves, wherein said a plurality of trenches and said plurality of source regions are arranged parallel to each other; 许多栅区,具有第2导电类型,每一个栅区设置在所述的底部;a plurality of gate regions, having a second conductivity type, each gate region is disposed on said bottom; 源电极,其中每一个源电极设置在所述许多源区中的相应一个源区上面;source electrodes, wherein each source electrode is disposed over a corresponding one of the plurality of source regions; 栅电极,其中每一个栅电极设置在所述许多栅区中的相应一个栅区上面;gate electrodes, wherein each gate electrode is disposed over a corresponding one of the plurality of gate regions; 第1和第2接触点,利用绝缘膜被设置在所述保护环区上面,并且连到所述源电极上;first and second contact points disposed above said guard ring region with an insulating film and connected to said source electrode; 第3接触点,利用所述绝缘膜设置在所述保护环区的所述公共部分上面,并连到所述栅电极。A third contact is provided on said common portion of said guard ring region by said insulating film, and is connected to said gate electrode. 12,按照权利要求11的静态感应晶体管,其特征是,所述第1,第2和第3接触点排成一直线(对准)。12. A static sensing transistor according to claim 11, wherein said first, second and third contacts are aligned (aligned). 13,按照权利要求11的静态感应晶体管,其特征是,所述许多源区和所述许多栅区与所述保护环区的一边相互垂直。13. The static induction transistor of claim 11, wherein said plurality of source regions and said plurality of gate regions are perpendicular to one side of said guard ring region. 14,按照权利要求11的静态感应晶体管、其特征是,所述第1和第2区相对于所述保护环区的公共部分是对称的。14. The static sensing transistor of claim 11 wherein said first and second regions are symmetrical with respect to a common portion of said guard ring region.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101266976B (en) * 2004-01-29 2010-06-16 三菱电机株式会社 Semiconductor device

Families Citing this family (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5903020A (en) * 1997-06-18 1999-05-11 Northrop Grumman Corporation Silicon carbide static induction transistor structure
US6750477B2 (en) * 1998-09-30 2004-06-15 Hitachi, Ltd. Static induction transistor
JP4017763B2 (en) * 1998-09-30 2007-12-05 株式会社ルネサステクノロジ Static induction transistor
US6750104B2 (en) * 2001-12-31 2004-06-15 General Semiconductor, Inc. High voltage power MOSFET having a voltage sustaining region that includes doped columns formed by trench etching using an etchant gas that is also a doping source
US6855970B2 (en) * 2002-03-25 2005-02-15 Kabushiki Kaisha Toshiba High-breakdown-voltage semiconductor device
JP4222092B2 (en) * 2003-05-07 2009-02-12 富士電機デバイステクノロジー株式会社 Semiconductor wafer, semiconductor device, and semiconductor device manufacturing method
JP5381420B2 (en) * 2008-07-22 2014-01-08 富士電機株式会社 Semiconductor device
US7825487B2 (en) * 2008-09-30 2010-11-02 Northrop Grumman Systems Corporation Guard ring structures and method of fabricating thereof
WO2011025973A1 (en) * 2009-08-28 2011-03-03 Microsemi Corporation Silicon carbide dual-mesa static induction transistor
US8519410B1 (en) 2010-12-20 2013-08-27 Microsemi Corporation Silicon carbide vertical-sidewall dual-mesa static induction transistor
US10224407B2 (en) 2017-02-28 2019-03-05 Sandisk Technologies Llc High voltage field effect transistor with laterally extended gate dielectric and method of making thereof

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5323029A (en) * 1992-03-04 1994-06-21 Zaidan Hojin Handotai Kenkyu Shinkokai Static induction device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4364072A (en) * 1978-03-17 1982-12-14 Zaidan Hojin Handotai Kenkyu Shinkokai Static induction type semiconductor device with multiple doped layers for potential modification
US5426314A (en) * 1992-07-29 1995-06-20 Zaidan Hojin Handotai Kenkyu Shinkokai Insulated gate control static induction thyristor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5323029A (en) * 1992-03-04 1994-06-21 Zaidan Hojin Handotai Kenkyu Shinkokai Static induction device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101266976B (en) * 2004-01-29 2010-06-16 三菱电机株式会社 Semiconductor device

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